Page 46 - Anatomy of a Robot
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02_200256_CH02/Bergren  4/17/03  11:23 AM  Page 31
                                   Moving mass (kinetic energy)
                                                                The energy in a moving mass is
                                                       E     0.5     m     v 2    CONTROL SYSTEMS 31
                                   where m is the mass, which will be described later in the book. v is the velocity.
                                   Note that a moving mass might not just be moving linearly. It might also be
                                   rotating. As such, you can model the energy of both motions separately. You can
                                   use the center of gravity of the mass and see how fast that is moving linearly.
                                   Then you can add the energy of rotation about that center of mass (as you find
                                   it).
                                   Mass at heights (potential energy) When a mass is at a height, the potential
                                   energy it has is given by the equation

                                                        E     m     g     h
                                                                                               2
                                   where M is its mass. g is the acceleration constant of gravity (32 ft/sec ). h is
                                   the height the mass might fall. A nice treatment of potential and kinetic energy
                                   can be found at www.dcate.net/coasters/pe.html.
                                Force evaluation  Instead of looking at energy, we’re going to use the technique
                                 of looking at everything in terms of force. We need only to characterize the forces
                                 within the system as they act together. In this way, we can predict what the pieces
                                 of the robot will do. Here are some of the places force is stored in a robot:
                                   Motor force  Most motors will generate a time-varying force when energy is
                                   applied. The force might be rotational or linear. To keep matters simple, we’ll
                                   be looking at linear force, such as might be applied by a solenoid, which is an
                                   electromagnet with a moving metal core, much like Figure 2-23.
                                   Moving mass force (kinetic force)  Newton created the equation for force
                                   acting on a mass (or mass creating a force):
                                                          F     m     A

                                   where m is the mass and A is the acceleration (or deceleration). When gravity
                                   is the force providing the acceleration, A   g and thus F   m   g, the force
                                   needed to hold up a mass m.
                                   Spring force  A spring with a spring constant of K will have a force

                                                           F     K     x
                                   where x is the compression (or elongation) of the spring.
                                   Friction force  Friction is a force that is engendered by velocity through a
                                   friction medium. For example, a motor, when the power is turned off, will cause
                                   the vehicle to coast to a stop because its rotor glides over the bearings and the
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